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Original Articles

Validation of hybrid angular spectrum acoustic and thermal modelling in phantoms

, , ORCID Icon & ORCID Icon
Pages 578-590 | Received 13 Feb 2018, Accepted 13 Aug 2018, Published online: 15 Oct 2018

Figures & data

Table 1. Parameters for acoustic and thermal simulations and their uncertainties for Monte Carlo analysis.

Figure 1. Experimental set-up for FUS sonications in homogeneous gelatin phantoms with real-time volumetric MRTI as shown in an axial T1-weighted MR image. (A) 256-element phased-array transducer is positioned below the phantom cylinder, coupled with room-temperature degassed, deionised water. The geometric focus was placed 19.5 mm into the base of the phantom. The MRTI image slab was oriented perpendicular to the direction of FUS beam propagation, with slices centred at the geometric focus. The base of the MRTI volume was 7.5 mm above the bottom of the phantom.

Figure 1. Experimental set-up for FUS sonications in homogeneous gelatin phantoms with real-time volumetric MRTI as shown in an axial T1-weighted MR image. (A) 256-element phased-array transducer is positioned below the phantom cylinder, coupled with room-temperature degassed, deionised water. The geometric focus was placed 19.5 mm into the base of the phantom. The MRTI image slab was oriented perpendicular to the direction of FUS beam propagation, with slices centred at the geometric focus. The base of the MRTI volume was 7.5 mm above the bottom of the phantom.

Table 2. Fixed acoustic and thermal simulation parameters and simulation computation time.

Figure 2. Average peak temperature rise achieved in the simulated (dashed, n = 1) and experimental (solid, n = 3) temperature profiles, with experimental error bars representing one standard deviation. Results are plotted as a function of milk concentration of the gelatin phantoms for both FUS sonication powers: 6.3 W (blue, circles) and 7.9 W (red, triangles).

Figure 2. Average peak temperature rise achieved in the simulated (dashed, n = 1) and experimental (solid, n = 3) temperature profiles, with experimental error bars representing one standard deviation. Results are plotted as a function of milk concentration of the gelatin phantoms for both FUS sonication powers: 6.3 W (blue, circles) and 7.9 W (red, triangles).

Table 3. Comparison of experimental (n = 3) and simulated (n = 1) temperature profiles at temporal peak of HIFU heating.

Figure 3. Transverse (top) and longitudinal (bottom) profiles of mean experimental (circle, black) and simulated (square, blue) temperature data in 50% milk composition phantoms at 7.9 W. Depicted transverse profiles are along the short-axis of the transducer face. For longitudinal profiles, the transducer is located to the left of the profiles. Experimental and simulated profiles are compared at multiple times points during heating (t = 3.04 and t = 9.76 s), at the time of experimental peak temperature rise (t = 16.48 s), and during cooling (t = 23.20 s and t = 29.92 s). Simulated profile resolution is down-sampled to 0.5 mm isotropic to match experimental spatial resolution.

Figure 3. Transverse (top) and longitudinal (bottom) profiles of mean experimental (circle, black) and simulated (square, blue) temperature data in 50% milk composition phantoms at 7.9 W. Depicted transverse profiles are along the short-axis of the transducer face. For longitudinal profiles, the transducer is located to the left of the profiles. Experimental and simulated profiles are compared at multiple times points during heating (t = 3.04 and t = 9.76 s), at the time of experimental peak temperature rise (t = 16.48 s), and during cooling (t = 23.20 s and t = 29.92 s). Simulated profile resolution is down-sampled to 0.5 mm isotropic to match experimental spatial resolution.

Figure 4. Average percent error in spatio-temporal peak temperature rise (black), transverse (blue, dashed) FWHM, and longitudinal (red, dotted) FWHM for all phantoms and sonication powers is plotted throughout FUS heating and cooling (n = 8; error bars= ± one standard deviation). The shaded regions represent time-points during which the average spatial SNR in the MRTI experimental data across all phantoms was ≤ 20.

Figure 4. Average percent error in spatio-temporal peak temperature rise (black), transverse (blue, dashed) FWHM, and longitudinal (red, dotted) FWHM for all phantoms and sonication powers is plotted throughout FUS heating and cooling (n = 8; error bars= ± one standard deviation). The shaded regions represent time-points during which the average spatial SNR in the MRTI experimental data across all phantoms was ≤ 20.

Figure 5. Temporal temperature curves of the peak temperature voxel from experimental (black, solid) and corresponding simulated (blue, dotted) temperatures for (a) 10%, (b) 30%, (c) 50%, and (d) 70% milk at 7.9 W sonication. Experimental error bars represent one standard deviation (n = 3). The shaded envelope represents one standard deviation of the MC analysis. The black dotted lines represent the high and low extremes of the MC analysis.

Figure 5. Temporal temperature curves of the peak temperature voxel from experimental (black, solid) and corresponding simulated (blue, dotted) temperatures for (a) 10%, (b) 30%, (c) 50%, and (d) 70% milk at 7.9 W sonication. Experimental error bars represent one standard deviation (n = 3). The shaded envelope represents one standard deviation of the MC analysis. The black dotted lines represent the high and low extremes of the MC analysis.

Table 4. Linear regression analysis of all MC Simulations (n = 568).

Figure 6. Output uncertainty (Uj) and relative output uncertainty (UjσXj) for three different output metrics of the MC simulations. (a) Uj when each parameter is varied individually (as specified in the legend). (b) UjσXj comparing the relative impact of each parameter on Uj. Output uncertainties were averaged over all phantoms and power levels. Error bars represent one standard deviation.

Figure 6. Output uncertainty (Uj) and relative output uncertainty (UjσXj) for three different output metrics of the MC simulations. (a) Uj when each parameter is varied individually (as specified in the legend). (b) UjσXj comparing the relative impact of each parameter on Uj. Output uncertainties were averaged over all phantoms and power levels. Error bars represent one standard deviation.